Non-reciprocal circuit element with a capacitor between the...

Wave transmission lines and networks – Plural channel systems – Nonreciprocal gyromagnetic type

Reexamination Certificate

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C333S024200

Reexamination Certificate

active

06215371

ABSTRACT:

TECHNICAL FIELD
The present invention relates to a non-reciprocal circuit element used in a microwave band radio device, for example in a mobile communication device such as a portable telephone.
BACKGROUND ART
In accordance with recent downsizing of mobile communication devices, demand for downsizing of non-reciprocal circuit elements such as isolators or circulators used in the communication devices has increased.
A conventional lumped element type circulator has an assembled circulator element with a circular plane shape and a basic structure as shown in an exploded oblique view of FIG.
1
.
In the figure, a reference numeral
100
denotes a circular substrate made of a non-magnetic material such as a glass-reinforced epoxy. Center conductors (inner conductors)
101
and
102
are formed on the top face and next to the bottom face of the non-magnetic material substrate
100
, respectively. These inner conductors
101
and
102
are electrically connected with each other by via holes
103
passing through the substrate
100
. Circularly shaped members
104
and
105
made of a ferromagnetic material are attached to the both faces of the non-magnetic material substrate
100
having the inner conductors
101
and
102
so that rotating RF (Radio Frequency) magnetic fluxes are induced In these ferromagnetic members
104
and
105
due to an RF power applied to the inner conductors
101
and
102
. The conventional circulator element of the circulator has a circular plane shape and is constructed by assembling, namely piling and bonding, the ferromagnetic members
104
and
105
on the both sides of the non-magnetic material substrate
100
.
The circulator as a whole is constructed, as shown in its exploded oblique view of
FIG. 2
, by stacking and fixing in sequence the ferromagnetic members
104
and
105
, grounding conductor electrodes
106
and
107
, exciting permanent magnets
108
and
109
and a metal housing separated to upper and lower parts
110
and
111
on the both side of the non-magnetic material substrate
100
having the inner conductors
101
(
102
), respectively. The housing parts
110
and
111
form a magnetic path of the magnetic flux from and to the exciting permanent magnets
108
and
109
.
If a RF power Is applied to the inner conductors
101
and
102
through terminal circuits not shown, RF magnetic flux rotating around the inner conductors
101
and
102
will be produced In the ferromagnetic members
104
and
105
. Under this state, If a dc magnetic field perpendicular to the RF magnetic flux is applied from the permanent magnets
108
and
109
, the ferromagnetic members
104
and
105
present different permeability &mgr;
+
and &mgr;

depending upon rotating sense of the RF magnetic flux, as shown in
FIG. 3. A
circulator utilizes this difference of the permeability depending upon the rotating sense. Namely, a propagation velocity of the RF signal in the circulator element will differ in accordance with the rotating sense and thus the signals transmitting to the opposite directions will cancel each other, thereby preventing the propagation of the signal to a particular port.
A non-propagating port is determined in accordance with its angle against a driving port due to the permeability &mgr;
+
and &mgr;

of the ferromagnetic member. For example, if ports A, B and C are arranged in this order along a certain rotating sense, the port B will be determined as the non-propagating port against the driving port A and the port C will be determined as the non-propagating port against the driving port B. Terminating one port of thus arranged circulator might constitute an isolator. Termination of the port can be realized by connecting to the port a matched resistor such as a chip resistor, or a thick or thin film resistor formed on a substrate for providing a resonance capacitor.
In such non-reciprocal circuit element, the ratio of volume occupied by the permanent magnet(s) is typically larger than that of another components. This has made difficult to downsize the non-reciprocal circuit element.
Most of conventional lumped element circulators may have a structure represented by an equivalent circuit shown in FIG.
4
. In this case, one end (outer conductor)
400
of each inductor of the circulator is directly connected to the ground.
Known in this field is, in order to widen frequency band of a circulator, to insert a serial resonance circuit
501
for adjusting eigen values of in-phase (equal phase) excitation between a common connection point (outer conductor)
500
to which one end of each inductor of the circulator is commonly connected and the ground, as shown in an equivalent circuit of FIG.
5
.
In general, to obtain three-port circulator operation, it is necessary to keep those admittances at in-phase excitation, positive phase excitation and negative phase excitation thereof have relationship of angular difference of 120 degrees with each other. The admittances at the positive phase excitation and the negative phase excitation will generally vary depending upon frequency change but admittance at the in-phase excitation will never change. Thus, if the frequency changes greatly, it is impossible to fees the relationship of angular difference of 120 degrees in the admittances causing that circulator operation cannot be expected. As a result, the operation frequency band of the circulator is limited to a narrower band.
Contrary to this, as aforementioned, by additionally inserting the serial resonance circuit for adjusting eigen values of in-phase excitation, the relationship of angular difference of 120 degrees in the admittances can be kept for a long time resulting the operation frequency band of the circulator to widen. However, the addition of the LC serial resonance circuit results of increase in the number of components of the circulator and therefore invites difficulty of downsizing of the circulator. In addition, since it is very difficult to make a small and high-performance inductor, the LC serial resonance circuit to be added will become large in size.
Japanese Patent Publication No.49(1984)-28219 discloses a circulator with capacitors each of which is inserted between one end of each inner conductor and the grounded conductor. An equivalent circuit of this circulator is shown in FIG.
6
. As will be understood from the figure, in the circulator, capacitors
601
,
602
and
603
are connected to respective ends of three inner conductors. However, according to this structure, these capacitors will exert an influence upon not only eigen values of In-phase excitation but also eigen values of both positive and negative phase excitations. Therefore, as well as the conventional art shown in
FIG. 4
, when the frequency changes greatly, it is impossible to keep the relationship of angular difference of 120 degrees in the admittances causing that circulator operation cannot be expected. As a result, the operation frequency band of the circulator is limited to a narrower band.
Temperature characteristics of the non-reciprocal circuit element will be discussed hereinafter.
There are various factors that will effect on the temperature characteristics of a non-reciprocal circuit element such as a circulator. It is considered that the main factor is temperature characteristics of saturation magnetization in the ferromagnetic material such as YIG (yttrium iron garnet) used for the circulator element, or the temperature characteristics of the permanent magnet(s) for providing bias magnetic field. In general, change in the temperature characteristics of the ferromagnetic material such as YIG used is larger than that of the bias magnetic field. Thus, the higher the temperature of the circulator, the higher its operation frequency becomes. This causes effective frequency band to be used to become narrower. Thus, in general, gadolinium is substituted in YIG to improve the temperature characteristics of saturation magnetization in YIG. However, the substitution of gadolinium causes loss of YIG to increase and therefore invit

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